JPS5931014B2 - distance measuring device - Google Patents
distance measuring deviceInfo
- Publication number
- JPS5931014B2 JPS5931014B2 JP12333980A JP12333980A JPS5931014B2 JP S5931014 B2 JPS5931014 B2 JP S5931014B2 JP 12333980 A JP12333980 A JP 12333980A JP 12333980 A JP12333980 A JP 12333980A JP S5931014 B2 JPS5931014 B2 JP S5931014B2
- Authority
- JP
- Japan
- Prior art keywords
- capacitor
- voltage
- distance measuring
- measuring device
- photodetector
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
Landscapes
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Semiconductor Lasers (AREA)
- Optical Radar Systems And Details Thereof (AREA)
Description
【発明の詳細な説明】
この発明はパルスレーザ光を用いた測距装置の改良に関
するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a distance measuring device using pulsed laser light.
パルスレーザ測距装置は、極めて時間幅の短い巨大レー
ザパルスを発生させ、それを測定しようとする目標物体
に向けて照射し、反射してきたレーザ光を受け、レーザ
光を投射してから受光までの時間を計測することによっ
て、目標までの距離を測定しようとするものである。Pulsed laser distance measuring equipment generates a gigantic laser pulse with an extremely short time width, irradiates it towards the target object to be measured, receives the reflected laser light, projects the laser light, and then processes the process until it is received. It attempts to measure the distance to the target by measuring the time.
まず従来のこの種装置の関連部分を第1図により説明す
る。First, related parts of a conventional device of this type will be explained with reference to FIG.
第1図において、1は充電電源、2は充電電源1の出力
を充電するコンデンサ、3はコンデンサ2の放電時にそ
の電流を制限するだめのチョークコイル、4はコンデン
サ2からの放電エネルギによりレーザ発振を行5レーザ
発振器、5は目標からのレーザ反射光を集光する受信光
学系、6は受信光学系5からの光を受は電気信号に変換
する光検知器、7は光検知器6の負荷抵抗、8は光検知
器6ヘバイアス駆動電圧を与える電源、9は出力信号を
増幅するビデオアンプである。In Figure 1, 1 is a charging power source, 2 is a capacitor that charges the output of the charging power source 1, 3 is a choke coil that limits the current when the capacitor 2 is discharged, and 4 is a laser oscillation due to the discharge energy from the capacitor 2. 5 is a laser oscillator, 5 is a receiving optical system that collects the laser reflected light from the target, 6 is a photodetector that receives the light from the receiving optical system 5 and converts it into an electrical signal, and 7 is a photodetector 6. A load resistor 8 is a power supply that applies a bias drive voltage to the photodetector 6, and 9 is a video amplifier that amplifies the output signal.
上記装置において、充電電源1からは所定のエネルギが
コンデンサ2に充電される。In the above device, a charging power source 1 charges a capacitor 2 with a predetermined amount of energy.
そのエネルギEは
■
E=−CV2(J)(1)
ここでC−コンデンサの容量(単位ファラド)V−充電
電圧(単位ボルト)
で示される。The energy E is expressed as: (1) E = -CV2 (J) (1) where C - capacitance of capacitor (unit: farad) V - charging voltage (unit: volt).
通常測距装置では、電圧として1000V前後が選ばれ
る。In a normal distance measuring device, a voltage of around 1000V is selected.
レーザ発振器4はコンデンサ2からの放電エネルギを受
けて、極めて時間幅の短い巨大パルス光を発生する。The laser oscillator 4 receives the discharge energy from the capacitor 2 and generates a huge pulsed light having an extremely short time width.
なおチョークコイル3は放電時のピーク電流を制限する
ために用いられている。Note that the choke coil 3 is used to limit the peak current during discharge.
このような構成で目標までの距離を測るためには、目標
に向けてレーザビームが発射され、距離に応じた時間遅
延をもって一部のレーザ光が反射してもどってくる。In order to measure the distance to a target with such a configuration, a laser beam is emitted toward the target, and some of the laser light is reflected back with a time delay depending on the distance.
その光は受信光学系5で集められ光検知器6に与えられ
る。The light is collected by a receiving optical system 5 and provided to a photodetector 6.
ところで最近のこの種装置ではレーザ発振素子としては
Nd(ネオジウム)をドープしたYAG(イツトリウム
、アルミニウム、ガーネット)の結晶が効率等の点から
使われることが多い。Incidentally, in recent devices of this kind, a YAG (yttrium, aluminum, garnet) crystal doped with Nd (neodymium) is often used as a laser oscillation element from the viewpoint of efficiency and the like.
その場合レーザ光の波長は1.06μmとなり近赤外の
不可視光線である。In this case, the wavelength of the laser light is 1.06 μm, which is near-infrared invisible light.
この場合光検知器としては感度等の点からシリコンを材
料としたAPD(アバランシェ、ホト、ダイオード)が
使われるのが一般的である。In this case, an APD (avalanche, photodiode) made of silicon is generally used as a photodetector in view of sensitivity and the like.
APDは電源8により逆バイアス電圧が与えられており
、通常その電圧は数百Vである。A reverse bias voltage is applied to the APD by a power source 8, and the voltage is usually several hundred volts.
光検知器6に光が加えられるとその強さに応じて受光電
流が流れ、負荷抵抗7に信号電圧として検出される。When light is applied to the photodetector 6, a light receiving current flows depending on the intensity of the light, and is detected as a signal voltage by the load resistor 7.
ビデオアンプ9は受信パルス信号を所定の大きさまで増
幅するためのものである。The video amplifier 9 is for amplifying the received pulse signal to a predetermined size.
測距装置としては第1図には示していないが、その他に
主要機能として計数回路があり、レーザ光が発射されて
から、受信信号が得られるまでの時間tを測定すること
により距離Rは、
−t
R−−(2)
ここでC二元の速度
で与えられる。Although not shown in Figure 1, the distance measuring device also has a counting circuit as its main function, which calculates the distance R by measuring the time t from when the laser beam is emitted to when the received signal is obtained. , -t R--(2) where it is given by the velocity of the C binary.
ところで、この種装置は携帯機器として使用されること
が多く装置は極力小型軽量であることが望ましい。Incidentally, this type of device is often used as a portable device, and it is desirable that the device be as small and lightweight as possible.
そのためには使用部品の数はできるだけ少く、電源等の
効率を極力高める必要がある。To achieve this, it is necessary to use as few parts as possible and to maximize the efficiency of the power supply, etc.
この発明はこのような観点に立ってなされたもので、従
来光検知器の駆動に用いていた電源を不用にし、代りに
レーザ発振に必要なコンデンサに充電された電荷を使用
するものである。The present invention was made from this point of view, and eliminates the need for a power source conventionally used to drive a photodetector, and instead uses the electric charge charged in a capacitor necessary for laser oscillation.
以下図面に従ってこの発明を説明する。The present invention will be explained below with reference to the drawings.
第2図はこの発明の一実施例を示すもので、第2図で充
電電源1、コンデンサ2、チョークコイル3、レーザ発
振器4、受信光学系5、光検知器6、負荷抵抗7、ビデ
オアンプ9は従来のものと同一である。FIG. 2 shows an embodiment of the present invention, in which a charging power source 1, a capacitor 2, a choke coil 3, a laser oscillator 4, a receiving optical system 5, a photodetector 6, a load resistor 7, a video amplifier 9 is the same as the conventional one.
10は電圧判定器、11はリレー、12はバイアスコン
デンサである。10 is a voltage judge, 11 is a relay, and 12 is a bias capacitor.
電圧判定器10はコンデンサ2の電圧が充電時上昇して
いるときはリレー11の接点を閉じ、バイアスコンデン
サー2も同様に充電させる。Voltage determiner 10 closes the contact of relay 11 when the voltage of capacitor 2 is rising during charging, and charges bias capacitor 2 in the same way.
そして光検知器6へのバイアス電圧が最適な値となった
ときリレー11を開き、コンデンサー2をコンデンサ2
から切シはなす。When the bias voltage to the photodetector 6 reaches the optimum value, the relay 11 is opened and the capacitor 2 is connected to the capacitor 2.
Cut the eggplant.
その動作の様子を第3図に示す。The operation is shown in Fig. 3.
通常レーザ測距装置は測距指令がくると、コンデンサ2
の充電を行い、それが所定の値に達つしたらレーザ発振
器4を駆動する。Normally, when a distance measurement command is received, a laser distance measurement device uses a capacitor 2.
is charged, and when it reaches a predetermined value, the laser oscillator 4 is driven.
光検知器6の動作電圧は上記充電電圧よりも低いところ
に選ばれ、受信光が入るまでほぼ一定値を保つ。The operating voltage of the photodetector 6 is selected to be lower than the charging voltage, and remains approximately constant until receiving light enters.
光検知器6としてAPD等を使用する場合、そのバイア
ス電流は極めて小さい。When an APD or the like is used as the photodetector 6, its bias current is extremely small.
また測距装置は通常ある一点の目標を測るため基本的に
パルス光の光電変換ができれば良い。Furthermore, since a distance measuring device usually measures a single target, it basically only needs to be capable of photoelectric conversion of pulsed light.
したがってその電源としては、測距ごとに充電を行った
コンデンサでまったく支障はない。Therefore, as a power source, a capacitor charged every time distance measurement is sufficient.
また電圧判定器10は通常のIC等のコンパレータを使
用して容易に実現できる。Further, the voltage determiner 10 can be easily realized using a comparator such as an ordinary IC.
以上説明したようにこの発明によれば、従来の、特に携
帯装置で一次電源としての電池から数百Vの電圧を作り
出す電源が不用となり、よシ軽量化が図れると共に待機
時にもそのままでは電池の電力を消費するということが
改善された装置を提供することができる。As explained above, according to the present invention, there is no need for a conventional power source that generates a voltage of several hundred volts from a battery as a primary power source, especially in a portable device, and it is possible to significantly reduce the weight of the device, and even when the device is on standby, the battery cannot be used as it is. A device with improved power consumption can be provided.
なお、実施例で用いたリレー11のかわりに、サイリス
タを用い、サイリスタの導通制御を行うゲートを電圧判
定器10で制御して実現できることはいうまでもない。It goes without saying that the present invention can be realized by using a thyristor instead of the relay 11 used in the embodiment and by controlling the gate for controlling conduction of the thyristor with the voltage determiner 10.
更には、充電電流を制限する抵抗と逆流防止ダイオード
を直列につないでリレー11の位置に用いることでも実
現できる。Furthermore, it can also be realized by connecting a resistor that limits the charging current and a backflow prevention diode in series and using the same at the relay 11 position.
この場合はレーザビームが発振されるまでにバイアスコ
ンデンサー12に所定の電圧が蓄積されるように抵抗値
を選択する。In this case, the resistance value is selected so that a predetermined voltage is accumulated in the bias capacitor 12 before the laser beam is oscillated.
従って、電圧判定器10を用いないで実現できる。Therefore, it can be realized without using the voltage determiner 10.
第1図は従来の測距装置を示すブロック図、第2図はこ
の発明の測距装置の一実施例を示すブロック図、第3図
はこの発明の測距装置の動作を説明する図である。
図において、1は充電電源、2はコンデンサ、3はチョ
ークコイル、4はレーザ発振器、5は受信光学系、6は
光検知器、7は負荷抵抗、8は電源、9はビデオアンプ
、10は電圧判定器、11はリレー、12はバイアスコ
ンデンサである。
なお図中同一あるいは相当部分には同一符号を付して示
しである。FIG. 1 is a block diagram showing a conventional distance measuring device, FIG. 2 is a block diagram showing an embodiment of the distance measuring device of the present invention, and FIG. 3 is a diagram explaining the operation of the distance measuring device of the present invention. be. In the figure, 1 is a charging power supply, 2 is a capacitor, 3 is a choke coil, 4 is a laser oscillator, 5 is a receiving optical system, 6 is a photodetector, 7 is a load resistor, 8 is a power supply, 9 is a video amplifier, and 10 is a A voltage judge, 11 is a relay, and 12 is a bias capacitor. In the drawings, the same or corresponding parts are designated by the same reference numerals.
Claims (1)
るコンデンサと、コンデンサに蓄えたエネルギの放電に
よシパルスレーザビームを発生するレーザ発振器と、レ
ーザビームの目標からの反射光を受光し電気信号に変換
する光検知器とから成り、目標布の距離を計測する測距
装置において、上記光検知器の駆動電圧を上記コンデン
サ蓄積エネルギから得ることを特徴とする測距装置。1. A power source that generates high voltage, a capacitor that stores the power output energy, a laser oscillator that generates a cipher laser beam by discharging the energy stored in the capacitor, and an electric signal that receives the reflected light from the target of the laser beam. What is claimed is: 1. A distance measuring device for measuring the distance to a target cloth, characterized in that a driving voltage for the photodetector is obtained from the energy stored in the capacitor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12333980A JPS5931014B2 (en) | 1980-09-05 | 1980-09-05 | distance measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12333980A JPS5931014B2 (en) | 1980-09-05 | 1980-09-05 | distance measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5746172A JPS5746172A (en) | 1982-03-16 |
| JPS5931014B2 true JPS5931014B2 (en) | 1984-07-30 |
Family
ID=14858111
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12333980A Expired JPS5931014B2 (en) | 1980-09-05 | 1980-09-05 | distance measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5931014B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2019204438A1 (en) * | 2018-04-17 | 2019-10-24 | Continental Automotive Systems, Inc. | Crosstalk mitigation circuit for lidar pixel receivers |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| AU1684883A (en) * | 1982-08-06 | 1984-02-09 | Emhart Industries Inc. | Inspection of glassware containers |
| JP2619661B2 (en) * | 1987-10-30 | 1997-06-11 | 株式会社光電製作所 | Laser pulse generator |
-
1980
- 1980-09-05 JP JP12333980A patent/JPS5931014B2/en not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2019204438A1 (en) * | 2018-04-17 | 2019-10-24 | Continental Automotive Systems, Inc. | Crosstalk mitigation circuit for lidar pixel receivers |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5746172A (en) | 1982-03-16 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP7584561B2 (en) | How to transmit power wirelessly | |
| US10557703B2 (en) | Distance measuring device and method for determining a distance | |
| US20180261975A1 (en) | Laser driver | |
| EP1132725B1 (en) | Monolithic circuit of active quenching and active reset for avalanche photodiodes | |
| US3815994A (en) | System and method for measuring distance | |
| JPH09189768A (en) | Laser distance measuring device receiver | |
| KR20140018402A (en) | Single photon detector in the near infrared using an ingaas/inp avalanche photodiode operated with a bipolar rectangular gating signal. | |
| CA2393514A1 (en) | Photodetector and method for detecting radiation | |
| US20180164412A1 (en) | LiDAR Apparatus | |
| CN112098973A (en) | Optical receiving device for lidar, dynamic adjustment method of optical receiving device | |
| Hallman et al. | A high-speed/power laser transmitter for single photon imaging applications | |
| US20180164410A1 (en) | LiDAR Apparatus | |
| US20190124748A1 (en) | Adaptive transmit light control | |
| US3937575A (en) | Electro-optical ranging means | |
| CN101545810A (en) | High-speed single photon detection method and detector | |
| US20160091617A1 (en) | Photon detection apparatus and associated methodology to enable high speed operation | |
| JPS5931014B2 (en) | distance measuring device | |
| US4939476A (en) | Laser Rangefinder receiver preamplifier | |
| JPH0412289A (en) | Pulse type laser range finder | |
| CN112394335A (en) | Laser range finder circuit of wide region power supply | |
| Liu et al. | A novel quenching circuit to reduce afterpulsing of single photon avalanche diodes | |
| JPH04307387A (en) | Range finder device | |
| KR920004499Y1 (en) | Infrared circuit | |
| JPS5949638B2 (en) | Dimming smoke detector | |
| Tsitomeneas | Optoelectronic indicator/warning circuit for detecting and observing the high values of incident optical radiation |